Ab initio calculation of the interaction potential for the krypton dimer: The use of bond function basis sets

1999 ◽  
Vol 111 (6) ◽  
pp. 2407-2413 ◽  
Author(s):  
Fu-Ming Tao
2010 ◽  
Vol 10 (3-6) ◽  
pp. 239-256
Author(s):  
Diego Paschoal ◽  
Marcello F. Costa ◽  
Georgia M.A. Junqueira ◽  
Hélio F. Dos Santos

1990 ◽  
Vol 45 (2) ◽  
pp. 184-188
Author(s):  
Saiful Islam ◽  
E. H. S. Anwander ◽  
M. M. Probst ◽  
B. M. Rode

AbstractAn analytical pair potential function for the system Cu(II)-water has been derived by means of ab initio calculation of the corresponding energy surface, using double zeta + polarization basis sets and effective core potentials. Tests on the function show that it should be reliable for use in Monte Carlo or molecular dynamics simulations.


1990 ◽  
Vol 43 (6) ◽  
pp. 1097 ◽  
Author(s):  
BN Figgis ◽  
PA Reynolds

We have performed ab initio discrete variational Xα calculations on a Cs18[Mo(NCS)6]15+ cluster, with the external electric field appropriate for a Cs3Mo(NCS)6 crystal. The calculations show both σ and π bonding, and also the participation of diffuse molybdenum- centred orbitals . Compared with the charge density experiment these effects are qualitatively correct but are underestimated. We performed further calculations successively removing the external electric field and the 18 Cs+ neighbours . The effects on the calculated metal- ligand bonding in the complex ion are negligible. This is not in agreement with experiment, so that these calculations which invoke only electrostatic effects and orthogonality with neighbouring ions and which also use only simple basis sets are not adequate. Further calculations on the Cr(NCS)63- and W(NCS)63- ions show increasing covalence from chromium to tungsten as expected. The spin transfer to the ligand is calculated to triple, but charge transfer is almost constant.


2001 ◽  
Vol 339 (5-6) ◽  
pp. 427-432 ◽  
Author(s):  
M.D Halls ◽  
H.B Schlegel ◽  
M.J DeWitt ◽  
G.W.F Drake

1992 ◽  
Vol 47 (3) ◽  
pp. 344-350 ◽  
Author(s):  
Hans-Ulrich Hummel ◽  
Thomas Fischer ◽  
Matthias Moll ◽  
Alexander Wolski ◽  
Peter Otto ◽  
...  

AbstractThe crystal structure of (AsPh4)2[Te(S2C = C(CN)2)2] has been determined by X-ray diffrac tion and the electronic structure has been calculated using an effective core potential approach for core electrons of Te and minimal basis-sets for valence electrons of Te and electrons of S, C and N. Te is situated in the center of planar [Te(S2C = C(CN)2)2]2- anions and is coordinated by four sulfur atoms in a trapezoid geometry with Te -S distances of 2.463(4), 2.524(4), 2.819(4) and 2.945(3) Å. The compound crystallizes in the triclinic space group P 1̄ with a = 9.562(5), b = 11.430(6), c = 27.319(20) Å, α = 93.248(2), β = 91.06(2), γ = 112.23(4)° and Z = 2. The trapezoid geometry allows a straightforeward mixing of Te 5 s-and one 5p-orbital giving rise to the formation of sp-hybride orbitals.


2010 ◽  
Vol 8 (3) ◽  
pp. 392-396 ◽  
Author(s):  
Herudi Kandau ◽  
Hanggara Sudrajat ◽  
Andreas Napitupulu ◽  
Syahrul Khairi ◽  
Zaky Al-Fatony ◽  
...  

Hydrogen bonded neutral clusters of ammonia, (NH3)n (n = 2-6), have been theoretically investigated employing the D95++(d,p) (and wherever necessary, higher) basis sets at the Hartree-Fock (HF) level as well as with second-order Møller-Plesset (MP2) perturbation theory. While the ammonia trimer and tetramer exhibit perfect molecular symmetries and are nonpolar, the pentamer and hexamer both optimize with slight deviations from perfect symmetries and are seen to posses marginal, but nonzero dipole moments. The (NH3)n linear clusters are seen to be chemically softer than the corresponding cyclic ones.   Keywords: ab initio calculation, ammonia clusters, Hartree-Fock, Møller-Plesset


2012 ◽  
Vol 67 (5) ◽  
pp. 411-416 ◽  
Author(s):  
Markus Luber ◽  
Arafa Musa ◽  
Hazem A. Kadry ◽  
Franz Bracher

The pyrrolizidine alkaloid intermedine-N-oxide was isolated from Cerinthe glabra for the first time. Due to the questionable assignments of NMR signals of this compound in previous literature reports ab initio calculations of the 13C NMR values based on the GIAO approach, using HF and B3LYP levels of theory and the four basis sets 6-31G(d), 6-311G(d), 6-31G(d,p), and 6-311G(d,p) were performed. The assignments obtained this way are in very good accordance with the experimental values.


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